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A calculation of the QCD phase diagram at finite temperature, and baryon and isospin chemical potentials

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arxiv hep-ph/0402104 v2 pith:XKXAWPOA submitted 2004-02-10 hep-ph

classification hep-ph
keywords chemicalisospinpotentialsbaryonfinitetemperatureanalysiscalculation
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We study the phases of a two-flavor Nambu-Jona-Lasinio model at finite temperature $T$, baryon and isospin chemical potentials: $\mu_{B}=(\mu_{u}+\mu_{d})/2$, $\mu_{I}=(\mu_{u}-\mu_{d})/2$. This study completes a previous analysis where only small isospin chemical potentials $\mu_{I}$ were considered

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Renormalization group invariant mean-field model for QCD at finite isospin density

    hep-ph 2025-02 conditional novelty 6.0 of 10

    A renormalization-group invariant mean-field quark-meson model with one fitted scale reproduces lattice QCD thermodynamics at finite isospin density and predicts a multicritical chiral/pion-condensation point in the c...

  2. Interplay between inhomogeneous chiral and crystalline color-superconducting phases in the two-flavor NJL model

    hep-ph 2026-06 unverdicted novelty 4.0 of 10

    In the two-flavor NJL model the wave vectors of the inhomogeneous chiral condensate and the single-plane-wave LOFF diquark condensate are never simultaneously nonzero, so the phases do not coexist.

  3. Minimal superfluid vortices in chiral perturbation theory

    hep-ph 2026-06 unverdicted novelty 4.0 of 10

    Leading order chiral perturbation theory yields the minimal energy condition for vortex nucleation in the pion condensed phase, with vortices carrying quantized angular momentum and self-confining pions.

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